X-Git-Url: https://git.lyx.org/gitweb/?a=blobdiff_plain;f=lib%2Fexamples%2Faas_sample.lyx;h=042fe8c043b261a5811653a096f120f7222ab330;hb=47b8ab14db71c6932ba5a8f159fc71a745792aca;hp=b1787b0c2b61d7fe0b6d549ade62cb007d361e71;hpb=8da26f548f51692d8fbe3598e3a0d2fe77967006;p=lyx.git diff --git a/lib/examples/aas_sample.lyx b/lib/examples/aas_sample.lyx index b1787b0c2b..042fe8c043 100644 --- a/lib/examples/aas_sample.lyx +++ b/lib/examples/aas_sample.lyx @@ -1,5 +1,5 @@ -#LyX 1.6.0svn created this file. For more info see http://www.lyx.org/ -\lyxformat 344 +#LyX 2.0 created this file. For more info see http://www.lyx.org/ +\lyxformat 413 \begin_document \begin_header \textclass aastex @@ -11,18 +11,26 @@ \shortauthors{Collapsed Cores in Globular Clusters} \end_preamble \use_default_options false +\maintain_unincluded_children false \language english +\language_package default \inputencoding default +\fontencoding global \font_roman default \font_sans default \font_typewriter default \font_default_family default +\use_non_tex_fonts false \font_sc false \font_osf false \font_sf_scale 100 \font_tt_scale 100 \graphics default +\default_output_format default +\output_sync 0 +\bibtex_command default +\index_command default \paperfontsize default \spacing single \use_hyperref false @@ -30,21 +38,31 @@ \use_geometry false \use_amsmath 0 \use_esint 0 +\use_mhchem 1 +\use_mathdots 1 \cite_engine basic \use_bibtopic false +\use_indices false \paperorientation portrait +\suppress_date false +\use_refstyle 0 +\index Index +\shortcut idx +\color #008000 +\end_index \secnumdepth 3 \tocdepth 3 \paragraph_separation indent -\defskip medskip +\paragraph_indentation default \quotes_language english \papercolumns 1 \papersides 1 \paperpagestyle default \tracking_changes false \output_changes false -\author "" -\author "" +\html_math_output 0 +\html_css_as_file 0 +\html_be_strict false \end_header \begin_body @@ -57,28 +75,22 @@ Collapsed Cores in Globular Clusters, Gauge-Boson Couplings, and AASTeX \begin_layout Author S. Djorgovski -\begin_inset ERT -status collapsed +\begin_inset Flex altaffilmark +status open \begin_layout Plain Layout - - -\backslash -altaffilmark{1,2,3} +1,2,3 \end_layout \end_inset and Ivan R. King -\begin_inset ERT +\begin_inset Flex altaffilmark status collapsed \begin_layout Plain Layout - - -\backslash -altaffilmark{1} +1 \end_layout \end_inset @@ -94,14 +106,11 @@ Astronomy Department, University of California, Berkeley, CA 94720 C. D. Biemesderfer -\begin_inset ERT +\begin_inset Flex altaffilmark status collapsed \begin_layout Plain Layout - - -\backslash -altaffilmark{4,5} +4,5 \end_layout \end_inset @@ -125,14 +134,11 @@ aastex-help@aas.org R. J. Hanisch -\begin_inset ERT +\begin_inset Flex altaffilmark status collapsed \begin_layout Plain Layout - - -\backslash -altaffilmark{5} +5 \end_layout \end_inset @@ -144,69 +150,85 @@ altaffilmark{5} Space Telescope Science Institute, Baltimore, MD 21218 \end_layout -\begin_layout Standard +\begin_layout Altaffilation +1 \begin_inset ERT -status open +status collapsed \begin_layout Plain Layout - -\backslash -altaffiltext{1}{Visiting Astronomer, Cerro Tololo Inter-American Observatory. - CTIO is operated by AURA, Inc. -\backslash - under contract to the National Science Foundation.} +}{ \end_layout -\begin_layout Plain Layout +\end_inset + +Visiting Astronomer, Cerro Tololo Inter-American Observatory. + CTIO is operated by AURA, Inc. +\begin_inset space \space{} +\end_inset +under contract to the National Science Foundation. \end_layout -\begin_layout Plain Layout +\begin_layout Altaffilation +2 +\begin_inset ERT +status collapsed +\begin_layout Plain Layout -\backslash -altaffiltext{2}{Society of Fellows, Harvard University.} +}{ \end_layout -\begin_layout Plain Layout +\end_inset +Society of Fellows, Harvard University. \end_layout -\begin_layout Plain Layout +\begin_layout Altaffilation +3 +\begin_inset ERT +status collapsed +\begin_layout Plain Layout -\backslash -altaffiltext{3}{present address: Center for Astrophysics, 60 Garden Street, - Cambridge, MA 02138} +}{ \end_layout -\begin_layout Plain Layout +\end_inset +present address: Center for Astrophysics, 60 Garden Street, Cambridge, MA + 02138 \end_layout -\begin_layout Plain Layout +\begin_layout Altaffilation +4 +\begin_inset ERT +status collapsed +\begin_layout Plain Layout -\backslash -altaffiltext{4}{Visiting Programmer, Space Telescope Science Institute} - +}{ \end_layout -\begin_layout Plain Layout +\end_inset +Visiting Programmer, Space Telescope Science Institute \end_layout -\begin_layout Plain Layout +\begin_layout Altaffilation +5 +\begin_inset ERT +status collapsed +\begin_layout Plain Layout -\backslash -altaffiltext{5}{Patron, Alonso's Bar and Grill} +}{ \end_layout \end_inset - +Patron, Alonso's Bar and Grill \end_layout \begin_layout Abstract @@ -455,8 +477,10 @@ A tree-level amplitude in \end_inset collisions can be expressed in terms of fermion strings of the form -\begin_inset Formula \begin{equation} -\bar{v}(p_{2},\sigma_{2})P_{-\tau}\hat{a}_{1}\hat{a}_{2}\cdots\hat{a}_{n}u(p_{1},\sigma_{1}),\end{equation} +\begin_inset Formula +\begin{equation} +\bar{v}(p_{2},\sigma_{2})P_{-\tau}\hat{a}_{1}\hat{a}_{2}\cdots\hat{a}_{n}u(p_{1},\sigma_{1}), +\end{equation} \end_inset @@ -516,29 +540,39 @@ In the chiral representation the \end_inset and the unit matrix 1 as -\begin_inset Formula \begin{eqnarray*} +\begin_inset Formula +\begin{eqnarray*} \gamma^{\mu} & = & \left(\begin{array}{cc} 0 & \sigma_{+}^{\mu}\\ -\sigma_{-}^{\mu} & 0\end{array}\right),\gamma^{5}=\left(\begin{array}{cc} +\sigma_{-}^{\mu} & 0 +\end{array}\right),\gamma^{5}=\left(\begin{array}{cc} -1 & 0\\ -0 & 1\end{array}\right),\\ -\sigma_{\pm}^{\mu} & = & ({\textbf{1}},\pm\sigma),\end{eqnarray*} +0 & 1 +\end{array}\right),\\ +\sigma_{\pm}^{\mu} & = & ({\textbf{1}},\pm\sigma), +\end{eqnarray*} \end_inset giving -\begin_inset Formula \begin{equation} +\begin_inset Formula +\begin{equation} \hat{a}=\left(\begin{array}{cc} 0 & (\hat{a})_{+}\\ -(\hat{a})_{-} & 0\end{array}\right),(\hat{a})_{\pm}=a_{\mu}\sigma_{\pm}^{\mu},\end{equation} +(\hat{a})_{-} & 0 +\end{array}\right),(\hat{a})_{\pm}=a_{\mu}\sigma_{\pm}^{\mu}, +\end{equation} \end_inset The spinors are expressed in terms of two-component Weyl spinors as -\begin_inset Formula \begin{equation} +\begin_inset Formula +\begin{equation} u=\left(\begin{array}{c} (u)_{-}\\ -(u)_{+}\end{array}\right),v={\textbf{(}}\vdag_{+}{\textbf{,}}\vdag_{-}{\textbf{)}}.\end{equation} +(u)_{+} +\end{array}\right),v={\textbf{(}}\vdag_{+}{\textbf{,}}\vdag_{-}{\textbf{)}}. +\end{equation} \end_inset @@ -558,9 +592,11 @@ The Weyl spinors are given in terms of helicity eigenstates \end_layout \begin_layout MathLetters -\begin_inset Formula \begin{eqnarray} +\begin_inset Formula +\begin{eqnarray} u(p,\lambda)_{\pm} & = & (E\pm\lambda|{\textbf{p}}|)^{1/2}\chi_{\lambda}(p),\\ -v(p,\lambda)_{\pm} & = & \pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi_{-\lambda}(p)\end{eqnarray} +v(p,\lambda)_{\pm} & = & \pm\lambda(E\mp\lambda|{\textbf{p}}|)^{1/2}\chi_{-\lambda}(p) +\end{eqnarray} \end_inset @@ -574,36 +610,46 @@ Floating material and so forth \begin_layout Standard Consider a task that computes profile parameters for a modified Lorentzian of the form -\begin_inset Formula \begin{equation} -I=\frac{1}{1+d_{1}^{P(1+d_{2})}}\end{equation} +\begin_inset Formula +\begin{equation} +I=\frac{1}{1+d_{1}^{P(1+d_{2})}} +\end{equation} \end_inset where -\begin_inset Formula \[ +\begin_inset Formula +\[ d_{1}=\sqrt{\left(\begin{array}{c} \frac{x_{1}}{R_{maj}}\end{array}\right)^{2}+\left(\begin{array}{c} -\frac{y_{1}}{R_{min}}\end{array}\right)^{2}}\] +\frac{y_{1}}{R_{min}}\end{array}\right)^{2}} +\] \end_inset -\begin_inset Formula \[ +\begin_inset Formula +\[ d_{2}=\sqrt{\left(\begin{array}{c} \frac{x_{1}}{PR_{maj}}\end{array}\right)^{2}+\left(\begin{array}{c} -\case{y_{1}}{PR_{min}}\end{array}\right)^{2}}\] +\case{y_{1}}{PR_{min}}\end{array}\right)^{2}} +\] \end_inset -\begin_inset Formula \[ -x_{1}=(x-x_{0})\cos\Theta+(y-y_{0})\sin\Theta\] +\begin_inset Formula +\[ +x_{1}=(x-x_{0})\cos\Theta+(y-y_{0})\sin\Theta +\] \end_inset -\begin_inset Formula \[ -y_{1}=-(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta\] +\begin_inset Formula +\[ +y_{1}=-(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta +\] \end_inset @@ -645,22 +691,8 @@ reference "tbl-2" \begin_inset Formula $M_{\sun}$ \end_inset -, but the assumption is that the alternate results should be less than 90 -\begin_inset ERT -status collapsed - -\begin_layout Plain Layout - - -\backslash -degr -\backslash - -\end_layout - -\end_inset - -out of phase with previous values. +, but the assumption is that the alternate results should be less than 90° + out of phase with previous values. We have no observations of \begin_inset ERT status collapsed @@ -751,8 +783,10 @@ Appendicial material \begin_layout Standard Consider once again a task that computes profile parameters for a modified Lorentzian of the form -\begin_inset Formula \begin{equation} -I=\frac{1}{1+d_{1}^{P(1+d_{2})}}\end{equation} +\begin_inset Formula +\begin{equation} +I=\frac{1}{1+d_{1}^{P(1+d_{2})}} +\end{equation} \end_inset @@ -760,25 +794,31 @@ I=\frac{1}{1+d_{1}^{P(1+d_{2})}}\end{equation} \end_layout \begin_layout MathLetters -\begin_inset Formula \[ +\begin_inset Formula +\[ d_{1}=\frac{3}{4}\sqrt{\left(\begin{array}{c} \frac{x_{1}}{R_{maj}}\end{array}\right)^{2}+\left(\begin{array}{c} -\frac{y_{1}}{R_{min}}\end{array}\right)^{2}}\] +\frac{y_{1}}{R_{min}}\end{array}\right)^{2}} +\] \end_inset -\begin_inset Formula \begin{equation} +\begin_inset Formula +\begin{equation} d_{2}=\case{3}{4}\sqrt{\left(\begin{array}{c} \frac{x_{1}}{PR_{maj}}\end{array}\right)^{2}+\left(\begin{array}{c} -\case{y_{1}}{PR_{min}}\end{array}\right)^{2}}\end{equation} +\case{y_{1}}{PR_{min}}\end{array}\right)^{2}} +\end{equation} \end_inset -\begin_inset Formula \begin{eqnarray} +\begin_inset Formula +\begin{eqnarray} x_{1} & = & (x-x_{0})\cos\Theta+(y-y_{0})\sin\Theta\\ -y_{1} & = & -(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta\end{eqnarray} +y_{1} & = & -(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta +\end{eqnarray} \end_inset @@ -788,8 +828,10 @@ y_{1} & = & -(x-x_{0})\sin\Theta+(y-y_{0})\cos\Theta\end{eqnarray} \begin_layout Standard For completeness, here is one last equation. -\begin_inset Formula \begin{equation} -e=mc^{2}\end{equation} +\begin_inset Formula +\begin{equation} +e=mc^{2} +\end{equation} \end_inset @@ -1140,16 +1182,7 @@ Spitzer, L. \end_layout \begin_layout Standard -\begin_inset ERT -status collapsed - -\begin_layout Plain Layout - - -\backslash -clearpage -\end_layout - +\begin_inset Newpage clearpage \end_inset @@ -1190,16 +1223,7 @@ This figure has no associated EPS file, so the optional parameter is omitted. \end_layout \begin_layout Standard -\begin_inset ERT -status collapsed - -\begin_layout Plain Layout - - -\backslash -clearpage -\end_layout - +\begin_inset Newpage clearpage \end_inset @@ -1238,9 +1262,10 @@ name "tbl-2" \end_layout \begin_layout Plain Layout +\align center \begin_inset Tabular - + @@ -1359,14 +1384,11 @@ Star \end_inset -\begin_inset ERT +\begin_inset Flex tablenotemark status collapsed \begin_layout Plain Layout - - -\backslash -tablenotemark{a} +a \end_layout \end_inset @@ -1410,14 +1432,11 @@ tablenotemark{a} \end_inset -\begin_inset ERT +\begin_inset Flex tablenotemark status collapsed \begin_layout Plain Layout - - -\backslash -tablenotemark{b} +b \end_layout \end_inset @@ -1832,14 +1851,11 @@ tableline \begin_layout Plain Layout -1.2 -\begin_inset ERT -status collapsed +\begin_inset Flex tablenotemark +status open \begin_layout Plain Layout - - -\backslash -tablenotemark{c} +c \end_layout \end_inset @@ -2000,14 +2016,11 @@ tablenotemark{c} \begin_layout Plain Layout 1.669 -\begin_inset ERT +\begin_inset Flex tablenotemark status collapsed \begin_layout Plain Layout - - -\backslash -tablenotemark{c} +c \end_layout \end_inset @@ -2198,48 +2211,78 @@ tablenotemark{c} \end_layout -\begin_layout Plain Layout +\begin_layout Table note +a \begin_inset ERT status collapsed \begin_layout Plain Layout +}{ +\end_layout -\backslash -tablenotetext{a}{Sample footnote for table~ -\backslash -ref{tbl-2} that was generated with the -\backslash -LaTeX -\backslash - table environment} +\end_inset + +Sample footnote for table +\begin_inset space ~ +\end_inset + + +\begin_inset CommandInset ref +LatexCommand ref +reference "tbl-2" + +\end_inset + + that was generated with the LaTeX table environment \end_layout +\begin_layout Table note +b +\begin_inset ERT +status collapsed + \begin_layout Plain Layout +}{ \end_layout -\begin_layout Plain Layout +\end_inset + +Yet another sample footnote for table +\begin_inset space ~ +\end_inset + + +\begin_inset CommandInset ref +LatexCommand ref +reference "tbl-2" + +\end_inset -\backslash -tablenotetext{b}{Yet another sample footnote for table~ -\backslash -ref{tbl-2}} \end_layout +\begin_layout Table note +c +\begin_inset ERT +status collapsed + \begin_layout Plain Layout +}{ \end_layout -\begin_layout Plain Layout +\end_inset +Another sample footnote for table +\begin_inset space ~ +\end_inset -\backslash -tablenotetext{c}{Another sample footnote for table~ -\backslash -ref{tbl-2}} -\end_layout + +\begin_inset CommandInset ref +LatexCommand ref +reference "tbl-2" \end_inset